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JPH0760640B2 - Microwave tube - Google Patents
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JPH0760640B2 - Microwave tube - Google Patents

Microwave tube

Info

Publication number
JPH0760640B2
JPH0760640B2 JP62166304A JP16630487A JPH0760640B2 JP H0760640 B2 JPH0760640 B2 JP H0760640B2 JP 62166304 A JP62166304 A JP 62166304A JP 16630487 A JP16630487 A JP 16630487A JP H0760640 B2 JPH0760640 B2 JP H0760640B2
Authority
JP
Japan
Prior art keywords
collector
magnetic field
frequency circuit
section
electron beam
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP62166304A
Other languages
Japanese (ja)
Other versions
JPS63146325A (en
Inventor
邦博 富川
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Priority to JP62166304A priority Critical patent/JPH0760640B2/en
Publication of JPS63146325A publication Critical patent/JPS63146325A/en
Publication of JPH0760640B2 publication Critical patent/JPH0760640B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Microwave Tubes (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、電子ビームを利用した進行波管などのマイク
ロ波管、特にそのコレクタ部の構造に関する。
Description: TECHNICAL FIELD The present invention relates to a microwave tube such as a traveling wave tube using an electron beam, and particularly to the structure of a collector portion thereof.

〔従来の技術〕[Conventional technology]

マイクロ波無線通信回線の中継局、衛星通信地上局など
の送信機に用いられるマイクロ波管においては、低消費
電力であることが要求されている。最近はマイクロ波管
以外の、装置各部の電力がIC化により低消費電力となっ
ているので、マイクロ波管に対する要求が格段と厳しく
なっている。
Low power consumption is required for microwave tubes used for transmitters such as relay stations of microwave radio communication lines and satellite communication ground stations. Recently, the power of each part of the equipment other than the microwave tube has become low power consumption due to the IC, so the demand for the microwave tube has become much more severe.

本発明の対象とするマイクロ波管は、電子銃部・高周波
回路部・コレクタ部および電子ビームを集束させる集束
磁界装置部から構成されるが、上記の低消費電力化の要
求に対しては、最も高周波特性に影響の少ないコレクタ
部について多段電位低下コレクタが考案されている。
The microwave tube of the present invention is composed of an electron gun part, a high frequency circuit part, a collector part, and a focusing magnetic field device part for focusing an electron beam, but in response to the above demand for low power consumption, A multi-stage potential drop collector has been devised for the collector part that has the least influence on the high frequency characteristics.

電子ビームは高周波回路と相互作用を行なう際、その結
合状態が各々異なり、相互作用後の電子ビームのもつ運
動エネルギーに分布が生じ速度分散を生じる。このよう
な速度分布のある電子ビームを、コレクタがすべて捕捉
するためには、その最も遅い電子ビーム群を捕捉するだ
けの電位としなければならない。しかし、それより早い
電子ビーム群の捕捉は、もともと上記電位より低くても
可能なのであるから、多段電位低下コレクタではコレク
タを数段にわけ、その電位を電子ビームの入射端から段
階的に下げて行くことで電子ビーム群を速度分別して捕
捉するようにしている。これによってコレクタの電位は
実効的に低下することになり、コレクタ損失を低減でき
る。
When the electron beam interacts with the high-frequency circuit, the coupling states thereof are different from each other, and the kinetic energy of the electron beam after the interaction has a distribution and velocity dispersion. In order for the electron beam having such a velocity distribution to be captured by the collector, the potential must be sufficient to capture the slowest electron beam group. However, since it is possible to capture an electron beam group earlier than that, even if the potential is originally lower than the above potential, the collector is divided into several stages in the multi-stage potential decreasing collector, and the potential is gradually lowered from the incident end of the electron beam. By going, the electron beam group is velocity-classified and captured. As a result, the collector potential is effectively lowered, and the collector loss can be reduced.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上記の多段電位低下コレクタでも、入射端の電位をさら
に低下しようとすると、コレクタに捕捉されるに十分な
速度をもたない一次電子ビーム群の一部分や、コレクタ
内面に発生した2次電子が、コレクタより高電位の高周
波回路部へ逆行し、高周波回路部に作用し、振幅歪・位
相歪など伝送特性に悪影響を及ぼし、また異常発振・動
作不安定になる。したがって多段電位低下コレクタで
も、その最高の電位を低下させるのに限界がある。
Even in the above-described multi-stage potential-decreasing collector, when the potential at the incident end is further reduced, a part of the primary electron beam group which does not have a velocity sufficient to be trapped by the collector and secondary electrons generated on the inner surface of the collector are It goes backward from the collector to the high-frequency circuit section having a higher potential, acts on the high-frequency circuit section, adversely affects the transmission characteristics such as amplitude distortion and phase distortion, and becomes abnormal oscillation and unstable operation. Therefore, even in the multi-stage potential decreasing collector, there is a limit in reducing the maximum potential.

また、多段電位低下コレクタ、あるいは一般のコレクタ
において、コレクタ電位の低下による逆行電子を防止す
るため、コレクタ外部にマグネットを取りつけることに
よってコレクタ内部に偏向用磁界を管軸に垂直に印加
し、電子軌道を曲げて、高周波回路部への逆行を防ぐ方
策をとることもある。しかし、強制空冷形マイクロ波管
等の場合は、コレクタの外周に熱伝導率の良い銅を材料
とする放熱翼を放射状にろう付した構造になっているの
で、放熱翼の外側から偏向用磁界を印加しても、放熱翼
の径方向の距離があるためコレクタ内部に発生する偏向
磁界は距離の2乗に反比例して弱くなる。そのため逆行
電子防止効果が小さくなってしまう欠点があった。
In order to prevent retrograde electrons due to a decrease in collector potential in a multi-stage potential decreasing collector or a general collector, a deflection magnetic field is applied inside the collector perpendicularly to the tube axis in order to prevent retrograde electrons due to a decrease in collector potential. There is also a possibility to take a measure to prevent the retrograde to the high frequency circuit section by bending. However, in the case of a forced air-cooled microwave tube, etc., a radiator blade made of copper with good thermal conductivity is radially brazed to the outer circumference of the collector, so that the deflection magnetic field is applied from the outside of the radiator blade. Even if is applied, the deflection magnetic field generated inside the collector becomes weak in inverse proportion to the square of the distance because of the radial distance of the heat radiating blade. Therefore, there is a drawback that the retrograde electron preventing effect becomes small.

本発明の目的は、多段電位低下コレクタあるいは一般の
コレクタにおいて、コレクタ電位低下により生ずる逆行
電子を有効に防ぐことによって、コレクタの電位を下げ
コレクタ損失を低下することのできるコレクタ部の構造
を有するマイクロ波管を提供することにある。
An object of the present invention is to provide a collector having a structure in which a collector portion can be lowered and collector loss can be reduced by effectively preventing retrograde electrons generated by the collector potential lowering in a multistage potential lowering collector or a general collector. To provide a wave tube.

〔問題点を解決するための手段〕[Means for solving problems]

本発明の対象であるマイクロ波管は、既に述べたよう
に、管軸方向に、電子銃部・高周波回路部・コレクタ部
が順に配置され、電子ビームは高周波回路部の全域にわ
たって設けられた集束磁界装置部の磁界により集束され
て高周波回路部を通過し、コレクタ部に捕捉されるよう
に構成されているものである。
As described above, the microwave tube which is the object of the present invention has the electron gun section, the high-frequency circuit section, and the collector section arranged in this order in the tube axis direction, and the electron beam is focused over the entire area of the high-frequency circuit section. It is configured such that it is focused by the magnetic field of the magnetic field device section, passes through the high-frequency circuit section, and is captured by the collector section.

本発明は、コレクタ部前縁のコレクタコアの一部に管軸
の垂直方向に、対称的に強磁性部材を対向して設け、該
対向強磁性部材を集束磁界装置の磁界により磁化し、電
子ビームに垂直な逆向き偏向磁界を形成するようにした
ものである。
According to the present invention, a ferromagnetic member is symmetrically opposed to a part of the collector core at the front edge of the collector portion in the direction perpendicular to the tube axis, and the opposed ferromagnetic member is magnetized by the magnetic field of the focusing magnetic field device to generate electrons. A reverse deflection magnetic field perpendicular to the beam is formed.

そのためには、コレクタコアに設けた強磁性部材を、極
力高周波回路部に近づけるとともに、強磁性部材の周縁
には、非磁性部材のみ配置し、集束磁界装置部の磁界が
シールドされないようにする。
For that purpose, the ferromagnetic member provided in the collector core is brought as close as possible to the high frequency circuit section, and only the non-magnetic member is arranged on the periphery of the ferromagnetic member so that the magnetic field of the focusing magnetic field device section is not shielded.

これによつて電子ビームに垂直な充分の強さの偏向磁界
を形成することができる。
As a result, it is possible to form a deflection magnetic field having a sufficient strength perpendicular to the electron beam.

〔作用〕[Action]

第2図のように、偏向磁界は管軸から互いに逆方向な垂
直磁界として生じ、本発明の目的とする高周波回路部へ
の逆行電子を防ぐことができる。
As shown in FIG. 2, the deflection magnetic field is generated as vertical magnetic fields in mutually opposite directions from the tube axis, and it is possible to prevent retrograde electrons to the high-frequency circuit section which is the object of the present invention.

〔実施例〕〔Example〕

以下、図面を参照して、本発明の一実施例として、集束
磁界装置部の磁界を利用する場合につき説明する。第1
図は、管軸方向の縦断面図、第2図は第1図のAA′断面
図である。
Hereinafter, as an embodiment of the present invention, a case of utilizing a magnetic field of a focusing magnetic field device will be described with reference to the drawings. First
The figure is a longitudinal sectional view in the tube axis direction, and FIG. 2 is a sectional view taken along the line AA 'in FIG.

マイクロ波管は、管軸方向に電子銃部1,高周波回路部2,
コレクタ部4が配置してある。高周波回路部2をおおう
ように全域にわたって集束磁界装置部3が設けられ、電
子銃部1から放射された電子ビームを集束する。電子ビ
ームは高周波回路部2において、相互作用をうけ速度分
布のある電子ビームとしてコレクタ部4に入力する。
The microwave tube consists of an electron gun section 1, a high frequency circuit section 2, and
A collector unit 4 is arranged. A focusing magnetic field device unit 3 is provided over the entire area so as to cover the high-frequency circuit unit 2 and focuses the electron beam emitted from the electron gun unit 1. The high-frequency circuit section 2 receives the electron beam as an electron beam having a velocity distribution in the high-frequency circuit section 2 and enters the collector section 4.

本例では、コレクタ部4は一体型で、銅製のコレクタコ
ア5を絶縁環6によつて、高周波回路部2に近接して配
置し、第2図に示すようにコレクタコア5の前縁部に鉄
などの強磁性部材7が、管軸に垂直に対称に対向して設
けられている。強磁性部材7は、高周波回路部2に近接
しているので、集束磁界装置部3の磁界によって磁化さ
れ、第2図に示すように強磁性部材7を磁力線がとお
り、管軸の垂直方向に充分強い磁界が発生する。コレク
タ部4の電位を低下したため、コレクタコア5に捕捉さ
れなかった電子ビームの一部やコレクタコア5の内表面
に発生した2次電子で、より高い電位をもつ高周波回路
部2へ逆行する電子が、逆行の経路において、コレクタ
部4の前縁部に生じた前記した管軸垂直方向の磁界で曲
げられ、再びコレクタコア5に捕捉される。
In this example, the collector portion 4 is an integral type, and the copper collector core 5 is arranged in the vicinity of the high frequency circuit portion 2 by the insulating ring 6, and the front edge portion of the collector core 5 is arranged as shown in FIG. Further, a ferromagnetic member 7 made of iron or the like is provided so as to be symmetrically opposed to and perpendicular to the tube axis. Since the ferromagnetic member 7 is close to the high-frequency circuit unit 2, it is magnetized by the magnetic field of the focusing magnetic field device unit 3, and the magnetic field lines pass through the ferromagnetic member 7 as shown in FIG. 2 in the direction perpendicular to the tube axis. A sufficiently strong magnetic field is generated. Since the potential of the collector portion 4 is lowered, a part of the electron beam not captured by the collector core 5 or secondary electrons generated on the inner surface of the collector core 5 are electrons which go backward to the high frequency circuit portion 2 having a higher potential. Is bent by the magnetic field in the direction perpendicular to the tube axis generated at the front edge of the collector portion 4 in the reverse path, and is captured again by the collector core 5.

〔発明の効果〕〔The invention's effect〕

以上説明したように、本発明ではコレクタ部の入口にお
いて、コレクタコアの内部に管軸に対し垂直な面に、発
生した充分強い偏向磁界が、コレクタコア内部からの戻
り電子、2次電子に作用して、高周波回路部への逆流を
効果的に防止する。したがって、コレクタコアの電位を
高周波回路部の電位より充分低くとることが可能にな
り、消費電力の大幅低減ができる。
As described above, in the present invention, at the entrance of the collector portion, the sufficiently strong deflection magnetic field generated in the surface inside the collector core perpendicular to the tube axis acts on the return electrons and secondary electrons from the inside of the collector core. Thus, backflow to the high frequency circuit section is effectively prevented. Therefore, the potential of the collector core can be made sufficiently lower than the potential of the high frequency circuit section, and the power consumption can be greatly reduced.

【図面の簡単な説明】[Brief description of drawings]

第1図,第2図は本発明の一実施例で、それぞれ管軸方
向の縦断面図、AA断面図である。 1……電子銃部、2……高周波回路部、3……集束磁界
装置部、4……コレクタ部、5……コレクタコア、6…
…絶縁環、7……強磁性部材、
FIG. 1 and FIG. 2 show an embodiment of the present invention, and are a vertical sectional view and a sectional view taken along the line AA in the tube axis direction, respectively. 1 ... Electron gun part, 2 ... High frequency circuit part, 3 ... Focusing magnetic field device part, 4 ... Collector part, 5 ... Collector core, 6 ...
… Insulating ring, 7… Ferromagnetic material,

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】管軸方向に、電子銃部・高周波回路部・コ
レクタ部が順に配置され、高周波回路部の全域にわたっ
て設けられた集束磁界装置部の磁界により電子ビームが
集束されて高周波回路部を通過し、コレクタに捕捉され
るように構成されたマイクロ波管において、 コレクタ部のコレクタコア前縁の一部に、管軸の垂直方
向に、対称的に強磁性部材を対向して設け、該対向強磁
性部材を前記集束磁界装置の磁界により磁化し、電子ビ
ームに垂直な互いに逆向きの偏向磁界を形成することを
特徴とするマイクロ波管。
1. An electron gun section, a high-frequency circuit section, and a collector section are sequentially arranged in the tube axis direction, and an electron beam is focused by a magnetic field of a focusing magnetic field apparatus section provided over the entire area of the high-frequency circuit section, whereby the high-frequency circuit section is formed. In a microwave tube configured to pass through and be trapped by the collector, a part of the front edge of the collector core of the collector part is provided with ferromagnetic members symmetrically opposed to each other in the direction perpendicular to the tube axis, A microwave tube characterized in that the opposing ferromagnetic members are magnetized by the magnetic field of the focusing magnetic field device to form deflection magnetic fields perpendicular to the electron beam in mutually opposite directions.
JP62166304A 1986-07-30 1987-07-02 Microwave tube Expired - Fee Related JPH0760640B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62166304A JPH0760640B2 (en) 1986-07-30 1987-07-02 Microwave tube

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP18035586 1986-07-30
JP61-180355 1986-07-30
JP62166304A JPH0760640B2 (en) 1986-07-30 1987-07-02 Microwave tube

Publications (2)

Publication Number Publication Date
JPS63146325A JPS63146325A (en) 1988-06-18
JPH0760640B2 true JPH0760640B2 (en) 1995-06-28

Family

ID=26490729

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62166304A Expired - Fee Related JPH0760640B2 (en) 1986-07-30 1987-07-02 Microwave tube

Country Status (1)

Country Link
JP (1) JPH0760640B2 (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5853135A (en) * 1981-09-25 1983-03-29 Nec Corp Traveling-wave tube
JPS607148U (en) * 1983-06-27 1985-01-18 日本電気株式会社 traveling wave tube

Also Published As

Publication number Publication date
JPS63146325A (en) 1988-06-18

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